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A Kinetic Description of Morphing Continuum: The zeroth and first order approximation

A Kinetic Description of Morphing Continuum: The zeroth and first order approximation

Seminar:

A Kinetic Description of Morphing Continuum: The zeroth and first order approximation
Thursday, March 29, 2018
3:30PM – 5PM
POB 6.304

James M. Chen

The coupling between the intrinsic angular momentum and the hydrodynamic linear momentum has been known to be prominent in fluid flows involving physics across multiple length and time scales, e.g. turbulence, nonequilibrium flows and flows at micro-/nano-scale. Since the classical Navier-Stokes equations and Boltzmann’s kinetic theory are derived on the basis of monatomic gases or volumeless points, efforts to derive constitutive equations involving intrinsic rotation for fluids of polyatomic molecules have been found since the 1960s. One of the proposed continuum theories for polyatomic molecules was Morphing Continuum Theory (MCT). The theory was originally formulated under the framework of rational continuum mechanics and thermodynamic irreversible processes. The mathematically rigorous continuum mechanics presents a complete and closed set of governing equations, but leaves the physical meanings unexplained. Similar to the correlation between Boltzmann's kinetic theory and the classical continuum mechanics, an advanced kinetic theory involving the Boltzmann-Curtiss (B-C) distribution function and the B-C equation will be introduced for a morphing continuum. The method of the most probable distribution method is used to derive the Boltzmann-Curtiss distribution. The corresponding Boltzmann-Curtiss equations will be demonstrated to be the MCT governing equations without any dissipation terms, i.e. the system (flows with inner structures) is in equilibrium and at the Boltzmann-Curtiss distribution. A first-order approximation to the B-C distribution will be used to further derive the B-C transport equations. The corresponding governing equations will then be compared with the MCT equations. Furthermore, a path to reduce the presented MCT equations down to the classical N-S equations will be demonstrated and discussed.

Bio
Dr. James M. Chen is an Assistant Professor of Mechanical Engineering and the Steve Hsu Keystone Research Faculty Scholar at Kansas State University. He earned his B.S. at National Chung-Hsing University (2000), M.S. at National Taiwan University (2005) and Ph.D. in mechanical and aerospace engineering and applied mathematics (minor) at The George Washington University (2011). He joined Kansas State University as an Assistant Professor in 2015. Prior to joining K-State, he was a faculty at the Penn State University system (2012-2015). He has published more than 30 peer-reviewed journal articles in multiscale computational mechanics, fracture mechanics, theoretical & computational fluid dynamics and atomistic simulation for thermo-electro-mechanical coupling. He received the Young Investigator Award from Air Force Office of Scientific Research in 2017. His research at MCPL has been supported by AFOSR, NSF and NASA. His current interests are on the kinetic description of Morphing Continuum, compressible turbulence, supersonic/hypersonic flows, atomistic electrodynamics, triboelectricity and high-level programming.